Table A6.
Non-vanishing quartic energy derivatives Kssst with respect to and their symmetry relations60
Symmetry |
![]() ![]() |
![]() |
Group | N |
---|---|---|---|---|
![]() |
![]() |
![]() |
I, II | ![]() |
![]() |
I, II | ![]() |
||
![]() |
![]() |
![]() |
I, II | ![]() |
![]() |
![]() |
![]() |
I, II | ![]() |
![]() |
![]() |
![]() |
I, II | ![]() |
![]() |
![]() |
![]() |
II | ![]() |
![]() |
II | ![]() |
||
![]() |
![]() |
![]() |
II | ![]() |
![]() |
![]() |
![]() |
II | ![]() |
![]() |
![]() |
![]() |
II | ![]() |
ci is the subscript labelling the degenerate representation of mode i, for example ci = 1 for E or E1, ci = 2 for E2, etc. p is a non zero integer number and N indicates the order of the principal symmetry axis. For I and II Group classification see Table A1.